Deriving Biot-Savart's Law, kinda a math problem not really physics

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SUMMARY

The forum discussion focuses on deriving Biot-Savart's Law using a vector method, specifically addressing the challenges faced during the integration process. The user attempts to simplify the derivation by substituting variables and correcting the coordinate system, ultimately leading to the expression for the magnetic field, \vec{B} = \frac{\mu_0 I}{4\pi} \int \frac{-y d\vec{y} \hat{k}}{(x^2 + y^2)^{\frac{3}{2}}}. The discussion highlights the importance of correctly defining angles and coordinates, as well as the potential pitfalls of using inconsistent variable definitions. Participants suggest using Ampere's Law as an alternative approach, emphasizing the need for clarity in mathematical expressions.

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  • Familiarity with vector calculus and cross products
  • Proficiency in integration techniques, including trigonometric substitutions
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  • Explore the derivation of Biot-Savart's Law using different coordinate systems
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  • #31
Okay! Tex is fixed on first page, made some other minor substition fixed. BUt my x^2 still remains..
 
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  • #32
Use the approach you did in post #3...

I also TeX-ed up my solution; I'll post it in a little bit...
 
Last edited:
  • #33
flyingpig said:
Okay! Tex is fixed on first page, made some other minor substitution fixed. But my x^2 still remains..
The last I looked, you did have inconsistencies between the way θ is drawn in your figure and the way it's used in some of your equations.d\vec{s} = <0,d\vec{y},0>  should be  d\vec{s} = <0,dy,0>

\hat{r} = <\cos\theta,\sin\theta,0>  should be  \hat{r} = <\sin\theta,\cos\theta,0>

In general  \left|\vec{A}\times\vec{C}\right|=\left|\vec{A}\right|\left|\vec{C}\right|\sin\theta so your cross product should have sin θ, not cos θ.

Jumping down to one of your equations for B:

\vec{B} = \frac{\mu_0 I}{4\pi} \int \frac{-cos\theta d\vec{y} \hat{k}}{x^2 + y^2}

After the above corrections and sin θ = x/r, you should have:

\vec{B} = \frac{\mu_0 I}{4\pi} \int \frac{-\sin\theta dy \hat{k}}{x^2 + y^2}
=-\,\frac{x\mu_0 I}{4\pi}\,\hat{k}\, \int \frac{ dy }{(x^2 + y^2)^{3/2}}

x comes out of the integral because you're integrating over y, not x.​
 
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  • #35
This is going to sound unrelated, but how did you make that pdf that is so compatiable with LaTeX?
 
  • #36
jhae2.718 said:
Here's my solution:
View attachment 33843
I didn't do the integration, but my solution agrees with this.

But, I do think there is a problem with both solutions.

It's late, so I'll look at it tomorrow.

Below added in Edit:

The concern I have with my solution, is that the variable, y, was used in two distinct ways. The primary way was as the variable of integration. The other way y was used was as a coordinate for the point, P.

I intend to redo my solution using (x0, y0) for the coordinates of P.


.
 
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  • #37
flyingpig said:
This is going to sound unrelated, but how did you make that pdf that is so compatiable with LaTeX?

I used LaTeX :)

MikTeX 2.9 on Windows.

Source:
Code:
\documentclass[10pt,letterpaper]{article}
\usepackage[latin1]{inputenc}
\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{fullpage}
\usepackage{graphicx}
\usepackage{float}
\usepackage{xfrac}
\newcommand{\custpic}[4]{\begin{figure}[H]
	\begin{center}
		\includegraphics[width=#2\textwidth]{#1}
		\vspace{-15pt}
		\caption{#3}
		\vspace{-20pt}
		\label{#4}
	\end{center}
\end{figure}}

\begin{document}
\custpic{pf5}{.75}{Problem diagram}{pf}

Start with Eq. (\ref{bs}), the Biot-Savart Law:
\begin{equation}\label{bs}
	d\vec{B} = \frac{\mu_0}{4\pi}\frac{id\vec{s} \times \hat{r}}{r^2}
\end{equation} 
From the diagram:
\begin{align*}
	r = \sqrt{x^2 + y^2} \\
	x = r\sin(\theta) \\
	y = r\cos(\theta) \\
	d\vec{s} = d\vec{y} 
\end{align*}
Substitute into Eq. (\ref{bs}):
\begin{equation}
	d\vec{B} = \frac{\mu_0}{4\pi}\frac{id\vec{y} \times \hat{r}}{x^2 + y^2}
\end{equation}
Taking the cross product, $id\vec{y} \times \hat{r} = dy\sin(\theta) (-\hat{k})$. Substitute in:
\begin{equation}
	d\vec{B} = \frac{\mu_0 i}{4\pi}\frac{dy\sin(\theta)}{x^2 + y^2} (-\hat{k})
\end{equation} 
From above, $\sin(\theta) = \dfrac{x}{r}$:
\begin{equation}
	d\vec{B} = \frac{\mu_0 i}{4\pi}\frac{xdy}{\left(x^2 + y^2\right)^{\sfrac{3}{2}}} (-\hat{k})
\end{equation} 
Find $\vec{B}$ by taking the integral over the infinite line:
\begin{equation}
	\vec{B} = \frac{\mu_0 i}{4\pi}\int\limits_{-\infty}^{\infty}\frac{xdy}{\left(x^2 + y^2\right)^{\sfrac{3}{2}}} (-\hat{k})
\end{equation} 
\begin{equation}
	\vec{B} = 2 \frac{\mu_0 i}{4\pi}\int\limits_{0}^{\infty}\frac{xdy}{\left(x^2 + y^2\right)^{\sfrac{3}{2}}} (-\hat{k})
\end{equation} 
Integrate (I used Wolfram$|$Alpha) to get:
\begin{equation}
	\vec{B} = 2 \frac{\mu_0 i}{4\pi}\left[\frac{y}{x\sqrt{x^2 + y^2}}\right]_{0}^{\infty} (-\hat{k})
\end{equation} 
The indefinite integral evaluates to:
\begin{equation}
	\vec{B} = \frac{\mu_0 i}{2\pi x} (-\hat{k})
\end{equation}
We can confirm this using Ampere's Law (left as an exercise to the reader...)
\end{document}
 
  • #38
It's getting late here, I will recheck my math tomorrow, thank you to both of you very much. That sentence did not make any sense, but hopefully you understood my appreciation.
 
  • #39
How did you save the file so perfectly? Whenever I saved it as a pdf, and I try reopen it it says it can't read it.
 
  • #40
SammyS said:
...
The concern I have with my solution, is that the variable, y, was used in two distinct ways. The primary way was as the variable of integration. The other way y was used was as a coordinate for the point, P.
...
Simply use x0 for x, and use (y0 - y) for y.

\vec{B}(x_0,\,y_0)=-\,\frac{x_0\mu_0 I}{4\pi}\,\hat{k}\, \int \frac{ dy }{(x_0^2 + (y_0-y)^2)^{3/2}}

I think you may find it handy to evaluate the integral from y0 to y .
 
  • #41
flyingpig said:
How did you save the file so perfectly? Whenever I saved it as a pdf, and I try reopen it it says it can't read it.

You need to run latex on it.

SammyS said:
Simply use x0 for x, and use (y0 - y) for y.

\vec{B}(x_0,\,y_0)=-\,\frac{x_0\mu_0 I}{4\pi}\,\hat{k}\, \int \frac{ dy }{(x_0^2 + (y_0-y)^2)^{3/2}}

I think you may find it handy to evaluate the integral from y0 to y .

That is an excellent point, and is something I just glossed over.
 
  • #42
WHat dose that mean "run latex" over it...?
 
  • #43
If you have a version of LaTeX installed, open up the command prompt, change directory to the location where you have saved the file, and type:
Code:
pdflatex filename.tex
replacing filename with the actual filename.
 
  • #44
I am guessing LaTeX is not the same thing as MikTeX lol
 
  • #45
MikTeX is a LaTeX distribution. http://docs.miktex.org/faq/faq.html

Try a LaTeX editor like TeXniCenter, Texmaker, etc to actually write/compile the code if you don't like the CLI.
 

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